WO2013031865A1

WO2013031865A1 - High-efficiency power amplifier

Info

Publication number: WO2013031865A1
Application number: PCT/JP2012/071909
Authority: WO
Inventors: 仁宏神山; 亮石川; 本城　和彦
Original assignee: 国立大学法人電気通信大学
Priority date: 2011-08-29
Filing date: 2012-08-29
Publication date: 2013-03-07
Also published as: KR101802572B1; EP2752990A1; EP2752990A4; CN103765765A; US20140225671A1; JPWO2013031865A1; CN103765765B; JP5979559B2; US9257948B2; KR20140053253A

Abstract

This high-efficiency power amplifier is provided with a transistor and an output power processing circuit unit. Here, the transistor amplifies input power having a base angular frequency component in current or voltage, and outputs output power. The output power processing circuit unit is connected to the rear stage of the transistor. The output power processing circuit unit is provided with an output modulation circuit unit and an output harmonic processing circuit unit. Here, the output modulation circuit unit performs impedance matching in the base angular frequency component. The output harmonic processing circuit unit is formed so that, among the power outputs, a plurality of harmonic components, each having a plurality of harmonic angular frequencies that are integer multiples of the base angular frequency, are changed to reactive power. The output harmonic processing circuit unit is formed to achieve a change to reactive power by causing the phases of the current and voltage of the output power to intersect in at least one of the plurality of harmonic components.

Description

High efficiency power amplifier

The present invention relates to a power amplifier, and more particularly, to a power amplifier having improved power efficiency by suppressing the average power consumption of harmonics in the power amplifier.

In power amplification, improving power efficiency is important. When a power amplifier using a transistor amplifies power having a desired fundamental frequency, the transistor is a nonlinear element, and therefore, in addition to the fundamental wave component having the fundamental frequency, unnecessary harmonics having a frequency that is an integral multiple of the fundamental frequency. Ingredients are produced. When this unnecessary harmonic component is consumed in the power amplifier, the additional power efficiency of the power amplifier is lowered.

As a method for controlling harmonic components and suppressing reduction in added power efficiency, a method using class F amplification and inverse class F amplification is known. In class F amplification and inverse class F amplification, the voltage and current on the output side of the transistor are separated in the time domain. More specifically, in class F amplification, the voltage is a square wave, the current is a sine half wave, and the voltage and current alternate to zero level. On the contrary, in the reverse class F amplification, the current is a square wave, the voltage is a sine half wave, and the voltage and the current are alternately at a zero level.

FIG. 1A is a graph group showing an example of a time change in a current flowing into a transistor and a voltage generated at an output terminal of the transistor of the class F amplifier. Here, the current flowing into the transistor is, for example, a drain current, and the voltage generated at the output terminal of the transistor is, for example, a drain-source voltage. The graph group in FIG. 1A includes a first graph 1Ai that shows the current flowing into the transistor, and a second graph 1Av that shows the voltage generated at the output terminal of the transistor. In FIG. 1A, the horizontal axis indicates the passage of time with the period of the fundamental frequency as a unit, and the vertical axis indicates the amplitude of current and voltage. The current i _d (t) shown in the first graph 1Ai and the voltage v _ds (t) shown in the second graph 1Av are expressed by the following equation (1).

As shown in the example of FIG. 1A, in the transistor of the class F amplifier, when the drain-source voltage is generated, the drain current becomes zero level, and when the drain current is generated, the drain-source voltage is zero. It is formed to be a level. Therefore, the power consumed inside the transistor of the class F amplifier is zero, and the average power consumption is also zero. As a result, the class F amplifier can theoretically obtain 100% power efficiency. The same applies to the inverse class F amplifier.

In relation to the above, Patent Document 1 (Japanese Patent No. 4335633) discloses an invention relating to a class F amplifier circuit and an additional circuit for a class F amplifier. The class F amplifier circuit includes a transistor and a load circuit connected to the subsequent stage of the transistor. The load circuit includes a first reactance two-terminal circuit and a second reactance two-terminal circuit. Each impedance has a zero at even harmonics and a pole at odd harmonics as needed.

Patent Document 2 (Japanese Patent Laid-Open No. 2011-55152) discloses an invention relating to an amplifier circuit. The amplifier circuit includes a transistor, a harmonic processing circuit connected to the subsequent stage of the transistor, and a resonance circuit unit connected to the subsequent stage of the harmonic processing circuit. This transistor can be expressed as an equivalent circuit having a current source, a drain-source capacitance, and a drain inductance. This harmonic processing circuit has an n-stage ladder circuit in which each stage includes a parallel capacitor and a series inductor. Here, n is an integer of 1 or more. This resonance circuit unit has 2n + 1 resonators having different resonance frequencies. The resonance frequency of these 2n + 1 resonators is the frequency of n + 1 poles and n zeros formed between the drain output part of the transistor and the ground plane when the output part of the harmonic processing circuit is short-circuited. Each matches. Among these 2n + 1 resonators, the resonance frequency of the 2n resonators matches the frequency of the second to 2n + 1 harmonics.

Patent Document 3 (Japanese Patent Laid-Open No. 2011-66839) discloses an invention relating to a microwave harmonic processing circuit. The microwave harmonic processing circuit includes a serial transmission line and a plurality of parallel tip open stubs connected in parallel at one point to an output terminal of the serial transmission line. This serial transmission line has an input terminal connected to the output terminal of the transistor and a predetermined electrical length. Each of the plurality of parallel open end stubs has a predetermined electrical length with respect to higher harmonics of the second order and up to the nth order. Here, n is an arbitrary integer, and the total number of parallel tip open stubs is n-1. The microwave harmonic processing circuit includes a first transmission line layer, a second transmission line layer, a ground layer, and a via. The first transmission line layer is configured by connecting a serial transmission line and two parallel tip open stubs out of n−1 parallel tip open stubs at one connection point. The second transmission line layer is configured by connecting n-3 parallel tip open stubs excluding these two parallel tip open stubs at one connection point. The ground layer is disposed between the first transmission line layer and the second transmission line layer. The via electrically connects the connection point in the first transmission line layer and the connection point in the second transmission line layer.

Japanese Patent No. 4335633 JP 2011-55152 A JP 2011-66839 A

Thus, the class F amplifier and the inverse class F amplifier realize extremely excellent power efficiency. However, in reality, in order to completely separate the current and voltage, a large amplitude is required as a harmonic component, that is, a transistor with higher high-frequency performance is required. In addition, since the class F amplifier and the inverse class F amplifier are easily affected by circuit loss, it may be relatively difficult to realize the ideal state particularly in the microwave band.

An object of the present invention is to provide a high efficiency power amplifier that is relatively easy to realize even in a high frequency band including a microwave band.

Hereinafter, means for solving the problem will be described using the numbers used in the (form for carrying out the invention). These numbers are added to clarify the correspondence between the description of (Claims) and (Mode for Carrying Out the Invention). However, these numbers should not be used to interpret the technical scope of the invention described in (Claims).

The high efficiency power amplifier according to the present invention includes a transistor (10) and an output power processing circuit unit (30). Here, the transistor (10) amplifies input power having a fundamental angular frequency component in current and voltage, and outputs output power. The output power processing circuit unit (30) is connected to the subsequent stage of the transistor (10). The output power processing circuit unit (10) includes an output matching circuit unit (32) and an output harmonic processing circuit unit (31). Here, the output matching circuit section (32) performs impedance matching in the basic angular frequency component of the output power. The output harmonic processing circuit section (31) is formed so that reactive power is converted into a plurality of harmonic components each having a plurality of harmonic angular frequencies that are integer multiples of the fundamental angular frequency. The output harmonic processing circuit section (31) is formed so as to realize reactive power generation by orthogonalizing the phases of current and voltage in output power in at least one of a plurality of harmonic components.

In the high-efficiency power amplifier according to the present invention, an output power processing circuit unit for converting the harmonic component of the output power to reactive power is provided at the subsequent stage of the transistor. The output power processing circuit unit converts at least part of the harmonic components into reactive power by making the current and voltage phases orthogonal. Thereby, a highly efficient power amplifier can be realized relatively easily even in a high frequency band including a microwave band.

FIG. 1A is a graph group showing an example of a time change in a current flowing into a transistor and a voltage generated at an output terminal of the transistor of the class F amplifier. FIG. 1B is a graph group showing an example of temporal changes in the current flowing into the transistor and the voltage generated at the output terminal of the transistor when the phase is orthogonal for each harmonic. FIG. 2 is a circuit diagram showing a basic configuration of the high efficiency power amplifier according to the embodiment of the present invention. FIG. 3 is a circuit diagram showing an implementation example of the configuration of the high efficiency power amplifier according to the embodiment of the present invention. FIG. 4A is a plan view of an input power processing circuit unit according to an embodiment of the present invention. FIG. 4B is a plan view of an output power processing circuit unit according to an embodiment of the present invention. FIG. 5 is a Smith chart showing the results obtained by measuring the characteristics of the high efficiency power amplifier according to the embodiment of the present invention. FIG. 6 is a graph group showing the results of measuring the power efficiency in the 5.7 Ghz band of the high efficiency power amplifier according to the embodiment of the present invention.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS Embodiments for implementing a high efficiency power amplifier according to the present invention will be described below with reference to the accompanying drawings.

(Embodiment)
As a technique for suppressing the power consumption in the transistor, the current flowing into the transistor and the voltage generated at the output terminal of the transistor are separated in the time domain to reduce the power consumption by the transistor like a class F amplifier or an inverse class F amplifier. In addition to the method of making reactive power, a method of making reactive power by making the phases of harmonic current and voltage orthogonal is conceivable. In the high-efficiency power amplifier according to the present invention, the method of orthogonalizing the phase of the harmonic current and voltage is used in combination with the method of the class F amplifier or the inverse class F amplifier, or by using it alone. The harmonic power consumption is suppressed.

FIG. 1B is a graph group showing an example of temporal changes in the current flowing into the transistor and the voltage generated at the output terminal of the transistor when the phase is orthogonal for each harmonic. The graph group in FIG. 1B includes a first graph 1Bi that shows the current flowing into the transistor, and a second graph 1Bv that shows the voltage generated at the output terminal of the transistor. In FIG. 1B, the horizontal axis indicates the passage of time with the period of the fundamental frequency as a unit, and the vertical axis indicates the amplitude of current and voltage. The current i _d (t) shown in the first graph 1Bi and the voltage v _ds (t) shown in the second graph 1Bv are expressed by the following equation (2).

The above formula (2) represents a case where the phase difference “Φ” is zero in the following more realistic formula (3).

As shown in the example of FIG. 1B, there is no particular period for maintaining the zero level for both current and voltage. However, the time integration of the power consumption in the transistor obtained by integrating the current and voltage becomes zero, that is, a power amplifier having theoretically 100% power efficiency is obtained. However, in the high-efficiency power amplifier of the present invention, even if the phase difference between the current and the voltage is slightly deviated from the ideal value of ± 90 ° in each of the harmonics other than the desired fundamental wave, as will be described later. In addition, an extremely high power efficiency with a drain efficiency exceeding 90% in actual measurement was obtained.

FIG. 2 is a circuit diagram conceptually showing the basic structure of the high-efficiency power amplifier according to the embodiment of the present invention. The components of the high efficiency power amplifier shown in FIG. 2 will be described. The high-efficiency power amplifier shown in FIG. 2 includes a transistor 10, a power supply circuit unit 20, an output power processing circuit unit 30, an input unit 50, and an output unit 60.

The power supply circuit unit 20 includes a power supply 21 and an impedance circuit unit 22. The transistor 10 includes a drain 11, a gate 12, and a source 13. The output power processing circuit unit 30 includes an output harmonic processing circuit unit 31 and an output matching circuit unit 32.

In the example of FIG. 2, a GaN (gallium nitride) HEMT (High Electron Mobility Transistor) is used as the transistor 10, but the present invention is not limited to this example. For example, the transistor 10 may be a bipolar transistor, a MOS (Metal Oxide Semiconductor) FET (Field Effect Transistor), or the like. However, in that case, the surrounding circuits are changed as necessary.

The connection relation of the components of the high efficiency power amplifier shown in FIG. 2 will be described. The input unit 50 is connected to the gate 12 of the transistor 10. One end of the power source 21 is grounded. The other end of the power source 21 is connected to one end of the impedance circuit unit 22. The other end of the impedance circuit unit 22 is commonly connected to the drain 11 of the transistor 10 and the input unit of the output harmonic processing circuit unit 31. The source 13 of the transistor 10 is grounded. The output unit of the output harmonic processing circuit unit 31 is connected to the input unit of the output matching circuit unit 32. The output unit of the output matching circuit unit 32 is connected to the output unit 60. In FIG. 2, the output matching circuit unit 32 is grounded, but may not be grounded. Further, the output unit 60 may be connected to an external load 40 as shown in FIG.

The operation of the high efficiency power amplifier shown in FIG. 2 will be described. The transistor 10 receives input power having a basic angular frequency ω ₀ from the gate 12. The transistor 10 amplifies input power while being supplied with power from the power supply circuit unit 20, and outputs the amplified output power from the drain 11. Here, the current 2i flowing through the drain 11 in FIG. 2 indicates the output power current i _d (t). Similarly, in FIG. 2, the voltage 2v between the drain 11 and the source 13 is the output power voltage v _ds (t ).

At this time, the output power outputted from the transistor 10, not only the fundamental wave component having a fundamental angular frequency omega _0, contains harmonics component having an integer multiple of the angular frequency of the fundamental angular frequency omega ₀ It is common. If these harmonic components are consumed in the amplifier, the efficiency of the amplifier is reduced.

Therefore, the output harmonic processing circuit unit 31 according to the present embodiment is connected to the subsequent stage of the transistor 10 to make most of the harmonic components of the output power reactive power. In the example shown in FIG. 2, the output harmonic processing circuit unit 31 includes first to third harmonic processing circuit units. Here, the first harmonic processing circuit unit converts the second harmonic component having an angular frequency 2ω ₀ that is twice the basic angular frequency ω ₀ out of the output power to reactive power. Similarly, the second harmonic processing circuit unit converts reactive power to a third harmonic component having an angular frequency 3ω ₀ that is three times the basic angular frequency ω _{0 in} the output power. Further, the third harmonic processing circuit unit converts reactive power to a fourth harmonic component having an angular frequency 4ω ₀ that is four times the basic angular frequency ω _{0 in} the output power. Note that the reactive harmonics are not consumed inside the high-efficiency power amplifier, but are eventually output as fundamental wave components, so reactive power contributes to improved power amplification efficiency. Will do.

It should be noted that it is possible to freely select which harmonic components these harmonic processing circuit units generate reactive power, and the examples used in the above description do not limit the present invention. Since the amplitude for each harmonic greatly depends on the characteristics of the transistor 10, it is naturally desirable to preferentially select a harmonic having a large amplitude as a target for reactive power. If an extreme example is given, only even harmonic components may be made reactive power.

In the prior art, in order to suppress the power consumption of these harmonic components, a method of class F amplifier or inverse class F amplifier is used in which the voltage and current are alternately adjusted to zero level for each harmonic. ing. The present invention never denies this technique, but in order to further promote the suppression of harmonic components, a reactive power technique that adjusts the phase of voltage and current to be orthogonal for each harmonic, Introduce to some or all of the harmonics. That is, some of the harmonics selected as control targets are converted into reactive power by making the phase of voltage and current orthogonal, and the rest of the harmonics are generated in the transistor using the method of class F amplifier or inverse class F amplifier. Zero power consumption. For example, reactive power is generated by making the phase of the voltage and current orthogonal for the fourth and subsequent harmonic components, and for the second and third harmonic components, a transistor is used by using a class F amplifier or an inverse class F amplifier. The power consumption inside is reduced to zero. Alternatively, the odd-order (even-order) harmonic components are converted to reactive power by making the voltage and current phases orthogonal to each other, and the even-order (odd-order) harmonic components are used as a class F amplifier or an inverse class F amplifier. Is used to zero the power consumption in the transistor. Alternatively, all of the harmonics selected as the control target may be converted to reactive power by making the voltage and current phases orthogonal.

By mixing two types of methods for suppressing the power consumption of harmonic components, an effect of providing further freedom in the design of the output harmonic processing circuit unit 31 or the output power processing circuit unit 30 can be obtained. In particular, when a microstrip line is used for zero power consumption for class F amplification or inverse class F amplification, it may be necessary to collect a plurality of open-ended stubs at the same connection point. Geometrical difficulties can occur. Here, the position where the open-ended stub should be connected is converted into the electrical length of the desired fundamental wave component, and is at a distance of a quarter wavelength from the output part of the transistor 10 (drain 11 in the case of FIG. 3). is there. Strictly speaking, this distance is slightly shorter than a quarter wavelength in consideration of the parasitic capacitance of the transistor 10. However, when a microstrip line is used to make the current and voltage phases orthogonal, a plurality of open-ended stubs can be distributed to a plurality of connection points respectively arranged at arbitrary positions of the main line part 34. And geometrical difficulties are unlikely to occur in their arrangement.

The output matching circuit unit 32 performs impedance matching with the subsequent stage for the fundamental wave component of the output power. Since impedance matching is the same as in the prior art, further detailed description is omitted. However, the output matching circuit unit 32 may be integrated with the output harmonic processing circuit unit 31 to form the output power processing circuit unit 30 as necessary.

Ideally, the phase difference between current and voltage is maintained at ± 90 degrees in all harmonics by adjusting the phase to be orthogonal. In this case, the theoretical efficiency is 100%. However, in practice, it is assumed that some error is allowed in the phase difference by sacrificing some efficiency. The allowable range depends on the ratio between the amplitude of the fundamental wave and the amplitude of each harmonic.

If the phase difference of the fundamental wave component is zero, the DC input power may be increased. On the other hand, when the DC input power is a given condition, the phase difference of the fundamental component may be adjusted.

When the transistor 10 is considered as an equivalent circuit including an output equivalent current source, impedance matching is performed on the fundamental wave component of the output power so that the impedance viewed from the output equivalent current source on the load 40 side is conjugate to the fundamental wave. Be consistent. Further, by performing reactive power conversion on the harmonic component of the output power, the impedance of the output equivalent current source viewed from the load 40 becomes pure reactance in the harmonic component.

From the output equivalent current source of the transistor 10, the impedance of the output power processing circuit unit 30 viewed from the rear stage becomes pure reactance for the harmonic component subjected to reactive power, and direct-current input power for the fundamental component The power factor corresponding to the active power component equal to may be set.

FIG. 3 is a circuit diagram showing an implementation example of the high efficiency power amplifier according to the embodiment of the present invention. The high efficiency power amplifier of FIG. 3 is equivalent to the high efficiency power amplifier according to the embodiment of the invention shown in FIG. 2 with two modifications. The first modification is that the output power processing circuit unit 30 according to the embodiment of the present invention is embodied, and the output power processing circuit unit 33 is formed by a distributed constant circuit such as a microstrip line. The second change is that an input power processing circuit unit 70 formed of a distributed constant circuit such as a microstrip line is added between the gate 12 of the transistor 10 and the input unit 50.

In FIG. 3, the power source 21 and the external load 40 are omitted for the sake of simplicity. Other configurations in the high efficiency power amplifier according to the present embodiment are the same as those in the embodiment of the present invention shown in FIG.

FIG. 4A is a plan view of the input power processing circuit unit 70 according to the implementation example of the embodiment of the present invention. The input power processing circuit unit 70 illustrated in FIG. 4A includes a main line unit 71, an input fundamental wave matching circuit unit 72, and an input harmonic processing circuit unit 73. Here, the input fundamental wave matching circuit unit 72 and the input harmonic processing circuit unit 73 are open-ended stubs.

The main line portion 71 has one end connected to the input unit 50 and the other end connected to the gate 12 of the transistor 10. The input fundamental wave matching circuit unit 72 has one end connected to the main line unit 71. The input harmonic processing circuit unit 73 has one end connected to the main line unit 71. Here, in the main line portion 71, a connection portion to the input portion 50, a connection portion to the input fundamental wave matching circuit portion 72, a connection portion to the input harmonic processing circuit portion 73, the gate 12 of the transistor 10, Are connected in this order.

The input fundamental wave matching circuit unit 72 performs impedance matching for a fundamental wave component having a desired fundamental angular frequency ω ₀ in the input power supplied from the input unit 50.

The input harmonic processing circuit unit 73 responds to the feedback component to the input side of the transistor 10 through the feedback capacitance in the transistor 10 among the secondary harmonic components of the voltage generated on the output side of the transistor 10. Perform phase adjustment. Here, the reason for focusing on the second harmonic component is that, since the amplitude is large among the harmonic components excluding the fundamental component, it is generally expected that the effect is the largest. . Therefore, if there is a high-order harmonic having an amplitude larger than that of the second-order harmonic component, it is preferable to use this higher-order harmonic component as a target for phase adjustment instead of the second-order harmonic component. As described above, the input harmonic processing circuit unit 73 may handle higher-order harmonics than 2, and a plurality of input harmonic processing circuits for phase-adjusting a plurality of higher-order harmonic components. The part 73 may be provided. In the example of FIG. 4A, the input harmonic processing circuit unit 73 has a fan shape, but this is only an example and does not limit the present invention.

FIG. 4B is a plan view of the output power processing circuit unit 33 according to the implementation example of the embodiment of the present invention. The output power processing circuit unit 33 shown in FIG. 4B includes a main line unit 34, a first output harmonic processing circuit unit 35, a second output harmonic processing circuit unit 36, and a third output harmonic processing. A circuit unit 37 and an output fundamental wave matching circuit unit 38 are provided. Here, the first output harmonic processing circuit unit 35, the second output harmonic processing circuit unit 36, the third output harmonic processing circuit unit 37, and the output fundamental wave matching circuit unit 38 are respectively It is a tip open stub.

The main line section 34 has one end connected to the drain 11 of the transistor 10 and the other end connected to the output section 60. One end of each of the first output harmonic processing circuit unit 35, the second output harmonic processing circuit unit 36, and the third output harmonic processing circuit unit 37 is in the main line unit 34. Commonly connected to the common connection. The output fundamental wave matching circuit section 38 has one end connected to the main line section 34. Here, in the main line section 34, the connection section of the transistor 10 to the drain 11, the common connection section of the first to third output harmonic processing circuit sections 35 to 37, the output fundamental wave matching circuit section 38, And the connection part with the output part 60 are arranged in this order.

It should be noted that a plurality of output harmonic processing circuit sections 35 to 37 commonly connected to the common connection section and the main line section 34 extending on both sides of the common connection section are preferably made as much as possible in order to suppress mutual influences. It is desirable to be connected at an angle.

The result of manufacturing the input power processing circuit unit 70 shown in FIG. 4A and the output power processing circuit unit 33 shown in FIG. 4B and measuring the characteristics thereof will be described.

FIG. 5 is a Smith chart showing the results obtained by measuring the characteristics of the high efficiency power amplifier according to the implementation example of the embodiment of the present invention. The Smith chart of FIG. 5 shows a total of four

points

51a, 52a, 53a, and 54a representing theoretical values, and a total of four

points

51b, 52b, 53b, and 54b representing actual measurement locations. A point 51a represents the theoretical value of the fundamental wave component. Point 52a represents the theoretical value of the second harmonic component. A point 53a represents the theoretical value of the third harmonic component. Point 54a represents the theoretical value of the fourth harmonic component. A point 51b represents an actual measurement value of the fundamental wave component. A point 52b represents an actual measurement value of the second harmonic component. A point 53b represents an actual measurement value of the third harmonic component. A point 54b represents an actual measurement value of the fourth-order harmonic component.

From these

points

51b, 52b, 53b and 54b, the voltage Vn, the current In, and the phase difference θn between the voltage Vn and the current In can be read. Here, n represents an integer of 1 to 4, 1 represents the fundamental wave component, and 2 to 4 represents the second to fourth harmonic components. The following “Table 1” shows measured values of the voltage Vn, the current In, and the phase difference θn in each of the fundamental wave component and the second to fourth harmonic components. The following “Table 1” also shows fifth-order harmonic components not shown in the Smith chart of FIG.

As can be seen from “Table 1”, the absolute value of the phase difference between voltage and current is in the range of 86.7 ° to 99 ° for the 2nd to 4th harmonic components for which the reactive power of the output power is applied. In other words, that is, almost orthogonal. In other words, if the absolute value of the phase difference between the voltage and current is 90 °, the power factor becomes zero and the reactive power is completely reduced, but the second to fourth harmonic components are close to this state. However, this does not apply to the fifth harmonic component that is not subject to reactive power conversion. That is, if the absolute value of the phase difference between the voltage and current is zero or 180 °, the power factor is 100% and the active power is completely achieved, but the fifth harmonic component is close to this state. In addition, for the desired fundamental wave component, the absolute value of the phase difference between the voltage and current is 120.4 °, and it is confirmed that no reactive power is generated. This phase difference represents a state where active power and reactive power are mixed and can be said to be sufficiently effective in practice.

FIG. 6 is a graph group showing the results of measuring the power efficiency in the 5.7 Ghz band of the high efficiency power amplifier according to the implementation example of the embodiment of the present invention. The graph group in FIG. 6 includes first to third graphs 6a to 6c. The first graph 6a represents the output power P _out with respect to the input power P _{in in} decibels (dBm). Second graph 6b represents an additional power efficiency PAE of input power _{P in} in percent (%). The third graph 6c represents the drain efficiency eta _D with respect to the input power _{P in} in percent (%).

In the measurement of FIG. 6, a drain efficiency of 90.7% and an additional power efficiency of 79.5% were obtained in the 5.7 GHz band. This result is compared with the case of a power amplifier according to the prior art. The following “Table 2” shows the measurement results of the high efficiency power amplifier according to the implementation example of the embodiment of the present invention and the measurement results of the power amplifiers according to the first to fifth conventional techniques.

In the above “Table 2”, the first conventional technology is “P. Colantonio, F. Gianni, R. Giofre, E. Limiti, A. Serino, M. Peroni, P. Romanini, and C. Proietti,“ As described in A C-band high0 efficiency second-harmonic-tuned hybrid power amplifier in GaN technology ”, IEEE Trans. Micro. Theory.27. The second conventional technology is “Y. Hao, L. Yang, X. Ma, J. Ma, M. Cao, C. Pan, C. Wang, and J. Zhang,“ High-Performance MicroAlvesedGate-ResidentialGate-ResidentialGate-ResidentialGate. / AlN / GaN MOS-HEMT With 73% Power-Added Efficiency ”, IEEE Electron Device Let., Vol. 32, no. 5, pp. 626-628. May 2011”. The third conventional technology is “R. Negra, and W. Bachold,“ BiCMOS MMIC class-E power amplifier for 5 to 6 GHz wireless communication systems, ”Proc. 35th Eur. 2005, pp. 445-448. The fourth conventional technology is “Y. Tsuyama, K. Yamanaka, K. Namura, S. Chaki, and N. Shinohara,“ Internally-matched GaN HEMT High Efficient MT ”. "Works. Dig., Kyoto, Japan, May 2011, pp. 41-44." The fifth conventional technology is “K. Kuroda, R. Ishikawa, K. Honjo,“ Parasic compensation design technology for C-bandGaN HEMT class-T.F.E.T ”. No. 11, pp. 2741-2750, Nov. 2010. ”.

As can be seen from Table 2 above, when compared with drain efficiency, 79.9% (fifth prior art), which was the highest value in the prior art, is high efficiency according to the implementation example of the embodiment of the present invention. In power amplifiers, a significant improvement of more than 10% has been realized.

As another implementation example of the high efficiency power amplifier according to the embodiment of the present invention, there is a variation in which the following change is added to the high efficiency power amplifier according to the embodiment of the present invention shown in FIG. That is, the output power processing circuit unit is formed using a lumped constant circuit such as a capacitor or an inductance. Other configurations and operations of the high efficiency power amplifier according to this embodiment are the same as those of the embodiment of the present invention shown in FIG.

By making the above changes, the high-efficiency power amplifier according to the present embodiment can be easily used in a power transmission device or the like in a contactless charging system for an electric vehicle using a megahertz band.

Each embodiment of the present invention described above can be freely combined within a technically consistent range. For example, in the high efficiency power amplifier according to the implementation example of the embodiment shown in FIG. 3, the input power processing circuit unit and the output power processing circuit unit are used by using the lumped constant circuit described in the other implementation example of the embodiment. It may be formed.

Claims

A transistor that amplifies input power including a fundamental wave component having a fundamental angular frequency in current and voltage and outputs output power;
An output power processing circuit unit connected to the subsequent stage of the transistor,
The output power processing circuit unit is
An output matching circuit unit for impedance matching in the fundamental wave component of the output power;
Among the output power, comprising an output harmonic processing circuit portion formed so as to be reactive power a plurality of harmonic components each having a plurality of harmonic angular frequencies that are integer multiples of the fundamental angular frequency,
The output harmonic processing circuit unit is configured to realize the reactive power generation by making current and voltage phases orthogonal to each other in the output power in at least one of the plurality of harmonic components. High efficiency power amplifier.
The high efficiency power amplifier of claim 1.
The output harmonic processing circuit section is
A high-efficiency power amplifier comprising a phase adjustment circuit unit that realizes the reactive power generation in the harmonic component of the predetermined order by short-circuiting with a harmonic of the predetermined order.
The high efficiency power amplifier of claim 2.
The output harmonic processing circuit section is
It further comprises another phase adjustment circuit unit that realizes the reactive power conversion in the harmonic component of the other order by short-circuiting with the harmonic of the other order,
The output power processing circuit unit is
Further comprising a main line portion connected between the output portion of the transistor and a subsequent load;
The high-efficiency power amplifier, wherein the phase adjustment circuit unit and the other phase adjustment circuit are respectively connected to a plurality of connection points in the main line unit.
The high efficiency power amplifier according to any one of claims 1 to 3,
The impedance of the output equivalent current source of the transistor as viewed from the rear side of the output power processing circuit unit is conjugate-matched with respect to the fundamental component, and the harmonic component subjected to the reactive power conversion For high efficiency power amplifier with pure reactance.
The high efficiency power amplifier according to any one of claims 1 to 3,
From the output equivalent current source of the transistor, the impedance of the output power processing circuit unit viewed from the rear stage becomes pure reactance for the harmonic component subjected to the reactive power, and for the fundamental component A high-efficiency power amplifier set to a power factor equivalent to an active power component equal to the DC input power.
The high efficiency power amplifier according to any one of claims 1 to 3,
The plurality of harmonic components that are converted to reactive power are:
A second harmonic component having an angular frequency twice the fundamental angular frequency;
A third harmonic component having an angular frequency three times the fundamental angular frequency;
A high-efficiency power amplifier including a fourth-order harmonic component having an angular frequency four times the fundamental angular frequency.
The high efficiency power amplifier according to any one of claims 1 to 6,
The output harmonic processing circuit section is
In terms of at least one of the plurality of harmonic components, the at least one of the plurality of harmonic components is connected to a position that is a quarter wavelength away from the output portion of the transistor in terms of a substantial electrical length of the fundamental wave component. A high-efficiency power amplifier comprising an open-ended stub formed so that the amplitude of one of voltage or current in one harmonic component is zero level.
The high efficiency power amplifier according to any one of claims 1 to 7,
The output harmonic processing circuit section is
A high-efficiency power amplifier comprising a distributed constant circuit section that converts reactive power to at least one of the plurality of harmonics.
The high efficiency power amplifier according to claim 8.
The distributed constant circuit section is
A high-efficiency power amplifier including an open-ended stub having an electrical length of a quarter wavelength of a harmonic to be made reactive power.
The high efficiency power amplifier according to claim 8.
The distributed constant circuit section is
Comprising a plurality of open-ended stubs having an electrical length of ¼ wavelength in each of the plurality of harmonics to be reactively powered;
One end portion of each of the plurality of open end stubs is a high efficiency power amplifier commonly connected to one point in the output harmonic processing circuit portion.
The high efficiency power amplifier according to any one of claims 1 to 10,
An input power processing circuit connected to the previous stage of the transistor;
The input power processing circuit unit is
An input matching circuit unit for impedance matching of the fundamental wave power;
A high-efficiency power amplifier comprising: an input harmonic processing circuit unit that performs reactive power conversion in at least one of the plurality of harmonic powers.
The high efficiency power amplifier according to any one of claims 1 to 11,
The transistor is
GaN (gallium nitride) HEMT (high electron mobility transistor)
A high efficiency power amplifier comprising:
The high efficiency power amplifier according to any one of claims 1 to 12,
The output harmonic processing circuit section is
A high-efficiency power amplifier comprising a lumped constant circuit unit that converts at least one of the plurality of harmonic powers into reactive power.
The output harmonic processing circuit unit according to any one of claims 1 to 13.